Oscillator coupling to reduce spurious signals in receiver circuits

Abstract

A first receiver frequency reference is passively coupled to a second receiver by tapping a signal directly from the resonant element, such as a crystal, of an oscillator in the first receiver to drive the input of the second receiver. The sinusoidal signal from the resonant element is relatively free of harmonics and minimizes interference that could be caused by harmonics of a square wave signal coupling or an amplified signal. The oscillator of each receiver can be selectively enabled or disabled to allow the receiver to either generate or receive the frequency reference. This technique of coupling can be used to couple a frequency reference signal between integrated circuit receivers.

Description

RELATED APPLICATIONS

This application claims priority from U.S. provisional application No. 60/684,505 filed May 25, 2005 entitled “Method of coupling oscillators to reduce spurious signals in receiver circuits”, incorporated herein by reference.

BACKGROUND

1. Field of the Invention

The present invention relates to oscillators and specifically to coupling a common reference between two oscillator circuits.

2. Prior Art

In receiver circuits, it is common practice to buffer the crystal oscillator signal of a phase-locked loop (PLL) of a first receiver circuit and use the buffered version of the signal as the reference for the phase-locked loop (PLL) of a second receiver circuit. The buffer used is commonly a saturated amplifier with its output signal being almost a square wave. This square wave output has a high number of harmonics present and some of these harmonics can end up present in the band of the receiver or the band of the mixer's output. The transmission of the harmonic-rich signal between receivers over circuit board traces provides an opportunity for the signal to radiate. The harmonics of the buffered signal can be an interferer and detrimental to the system similar to unwanted signals picked up from the antenna.

FIG. 1 shows the prior art with the buffered oscillator signal being used as the reference for the second receiver circuit's PLL.

SUMMARY OF INVENTION

The crystal oscillator of a first phase-locked loop (PLL) of a first receiver circuit is coupled to a second PLL of a second receiver. This crystal oscillator is shared between the two receiver circuits without using a buffered oscillator signal as in the prior art. By avoiding the use of the buffer, the detrimental harmonics caused by the buffer are eliminated. The reference input buffer of the second receiver circuit is specified according to the amplitude available from the crystal circuit, providing a moderately high input impedance. The extra load capacitance introduced by the device being driven and by the board trace is taken in account during the design of the crystal oscillator circuit. The crystal oscillator (XO) can be of any topology, for example a Pierce crystal oscillator.

In the invention, the crystal oscillator of the second slave receiver is disabled. The oscillator is disabled in the slave device to avoid having the amplified version of the input signal radiating on the board which may cause similar detrimental harmonics as would the use of an output buffer in the prior art. The disabling of the oscillator can be achieved by using one P-type field-effect transistor (FET) and one N-type FET to couple power to the amplifier used in the crystal oscillators.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows the prior art with the crystal oscillator signal buffered prior to use in the second receiver circuit.

FIG. 2 shows a block diagram of oscillator coupling according to the present invention.

FIG. 3 shows detail of an oscillator circuit for use with the present invention.

DETAILED DESCRIPTION OF THE INVENTION

FIG. 2 shows a block diagram coupling an oscillator according to the present invention. Two receiver circuits are shown, master 100 and slave 200. Master 100 comprises crystal oscillator 110, phase-locked loop (PLL) and filter circuit 120, crystal oscillator (XO) input buffer 115, voltage controlled oscillator (VCO) 140, mixer 150 and low noise amplifier (LNA) 160. The crystal oscillator output buffer 130 would be used in the prior art method of coupling the oscillator signal to a second receiver. Capacitors 172 provide the capacitance to achieve the necessary requirement that the overall loop gain has zero (or 360) degrees phase shift at the oscillation frequency. The crystal 170 is connected such that it forms part of the feedback impedance of the inverting amplifier in the crystal oscillator circuit 110, which operates in a non-saturating linear or near linear mode.

Oscillator 110 drives receiver 200 through capacitor 180, which isolates the direct current bias of oscillator circuit 210 and passes only the oscillating signal. The signal is coupled between receivers passively, without the use of a buffer amplifier. The reference signal from oscillator 110 drives input buffer 215, an amplifier, to provide the reference signal to the PLL of receiver 200. When used as a slave device, crystal oscillator 210 is disabled and the reference signal is input at the disabled output terminal of the oscillator amplifier where input buffer 215 is connected. Input buffer 215 is active and drives the reference signal in receiver 200. A capacitor can optionally be connected to the input of oscillator circuit 210 to provide an AC ground at that terminal.

XO output buffers 130 and 230 can be disabled when using the configuration of the present invention. Although not required in the present invention, the XO output buffer can be included in the receiver circuit to provide compatibility with other devices that do not use the present inventive configuration.

The present circuit and method passively couples a reference oscillating signal between two receivers with a substantially sinusoidal waveform, which avoids coupling and radiation of harmonics of the fundamental waveform that could occur in a signal path between the two receivers. Internal clock signals derived from the reference signal and used in the receivers can be non-sinusoidal or square. The receivers can be implemented as single-chip devices with short internal signal paths that reduce the opportunity for radiation of harmonics that can occur in a long signal path.

FIG. 3 shows the topology of the crystal oscillator 110, using a Pierce topology. Other oscillator topologies can be used with this invention. The resonator is preferably a crystal, and can alternatively be an inductor and capacitor circuit. The crystal 170 is connected to the input 303 and output 309 of the active device, inverting amplifier 300, and provides the feedback impedance in parallel with resistor 301. In this configuration, the crystal is operating at or near its series resonant frequency and has low impedance.

The oscillator circuit may be disabled or enabled by the application of enable signal 304. The enable signal 304 is connected to the gate of a P-type field effect transistor (PFET) 306 and to the gate of an N-type field effect transistor (NFET) 307. When the enable signal is high, transistor 306 is active and power 305 is applied to the inverting amplifier 300. When the enable signal 304 is low, transistor 306 is off and transistor 307 is active resulting in a voltage difference of zero being applied to the power inputs of amplifier 300.

The oscillator circuit of the master receiver must be enabled to drive the slave circuitry, while the slave circuit has its oscillator circuit disabled. The selective enabling of the oscillator of the present invention allows identically fabricated devices to be used in a multiple receiver system with programming to select master and slave receivers.

The method of coupling oscillator circuits of the present invention provides component saving in a multiple oscillator circuit while maintaining a spectrally pure reference signal for the oscillators. The transmission of a harmonic-rich non-sinusoidal waveform between receiver devices is avoided. The method and apparatus of connecting receiver frequency references of the present invention can be extended to any number of recievers.

Claims

1. A method of coupling an oscillating signal from a first receiver to a second receiver comprising:

connecting a resonant element to a first oscillating circuit in the first receiver;

operating the first oscillating circuit in a non-saturating mode to produce a substantially sinusoidal waveform signal on the resonant element;

using the sinusoidal waveform signal as a frequency reference in the first receiver;

coupling the sinusoidal waveform signal present at the resonant element to a second oscillating circuit in the second receiver; and

using the coupled signal as a frequency reference in the second receiver.

2. The method of claim 1 wherein coupling the sinusoidal waveform is done passively without using a buffer amplifier.

3. The method of claim 2 wherein the coupling is performed with a capacitor.

4. The method of claim 1 wherein the resonant element comprises a piezoelectric crystal.

5. The method of claim 1 wherein the resonant element comprises an inductor and capacitor.

6. The method of claim 1 wherein the second receiver accepts the signal using an input amplifier and the second receiver comprises an oscillator circuit that is disabled.

7. The method of claim 6 further comprising:

selectively enabling power to the first and second oscillating circuits, wherein the second oscillating circuit is disabled and the first oscillating circuit is enabled.

8. A receiver device with an oscillator circuit that can selectively couple a frequency reference signal to another receiver device or receive a frequency reference from another device comprising:

a sinusoidal oscillator with an enable circuit;

an amplifier connected to the output of the oscillator for amplifying the frequency reference to drive receiver circuitry;

wherein in a first mode of operation the oscillator can be enabled and connected to a resonant element to create an oscillator and generate the frequency reference;

and in a second mode of operation the oscillator can be disabled and the receiver device receives the frequency reference at the output of the disabled oscillator.

9. The receiver device of claim 8 wherein in the first mode of operation the receiver device drives another like device through a passive coupling.

10. The receiver device of claim 9 wherein the passive coupling consists of a capacitor.

11. The receiver device of claim 8 wherein in the second mode of operation the receiver device receives the frequency reference by a passive connection to the resonant element of another like device.

12. The receiver device of claim 11 wherein the passive coupling consists of a capacitor.